Microwave impedance matching package for microwave cooking

Abstract: A food package (10) including a package body forming a food receiving cavity (14) for storing and heating a food item (12) in a microwave oven. Specifically, the package body includes a bottom panel (20) and a top panel (16) with side panels (18) joining the bottom and top panel. An impedance matching element (22) is provided on at least one of the panels for impedance matching microwave energy entering the package. The impedance matching element is preferably a contiguous film of thinly flaked material embedded in a dielectric binder which is sized and shaped with respect to the food to cause impedance matching to elevate the temperature of the food in predetermined areas dependent upon the size and spacing of the film without interacting with the microwave energy to produce heat. The film may also be shaped in the form of a convex lens to direct impedance matched microwave energy toward the food to elevate the temperature of the food in a predetermined area. Further, the flake material may be present in the binder in an amount sufficient to provide microwave shielding.

Description: The present invention relates to microwave cooking of a food item. More particularly, the present invention relates to a package for storing and microwave heating food according to the preamble of claim 1 and a method for producing such a package. The popularity of microwave ovens for cooking all or a part of a meal has led to the development of a large number of food packages capable of cooking a food item in a microwave oven directly in the food package in which it is stored. The convenience of cooking food in its own package or a component thereof appeals to a large number of consumers. However, one dissatisfaction of microwave cooking for some foods is the inability to heat or warm the center of the food without burning or severely dehydrating the exterior thereof. In particular, larger servings are very difficult to heat uniformly using conventional food packages in a microwave oven. Even when the outer portions are thoroughly cooked, the center is generally undesirably cool. Microwave interactive films have been produced which are capable of generating heat at the food surface to crispen some food products. US - A - 4,641,005 discloses a microwave interactive material useful in food packaging which is capable of browning the surface of a food item. Specifically, the interactive material includes a very thin metal film applied to a polymer material which is adhered to a rigid substrate. Such a film actually interacts with microwave energy to produce heat at the surface of the food. The heat provided by such an interactive material is advantageous for browning the surface of a food item, but is not advantageous for cooking a thick food item having a large dielectric constant because the outer portion of the food will cook even faster than without interactive material resulting in a deficiently heated inner portion. Additional microwave heating devices have also been developed primarily for use in food packaging. US - A - 4,876,423 discloses a medium for producing localized microwave radiation heating wherein the medium is formed from a mixture of polymeric binder and conductive and semiconductive particles that can be coated or printed on a substrate. Again, however, such a medium is designed to interact with the electromagnetic, microwave energy to produce heat and thereby, brown or crispen the surface of a food item, while providing no enhanced heating of the center of the food. A number of microwave food packages or containers have also been developed which are designed to uniformly heat or adjust the reflectance, transmittance, or absorbance of microwave energy. US - A - 4,266,108 discloses a microwave heating device which includes both a microwave reflective member and a microwave absorbing member spaced apart a distance sufficient to provide a temperature self-limiting device. As provided in the above-noted patents, however, the device includes a heater member which interacts with the microwave energy to produce heat and, thus, conductively heats the food item. Further, US - A - 4,927,991 is directed to a food package which discloses a susceptor or heater element in combination with a grid wherein the susceptor surface may be tuned to a matched impedance for maximum microwave power absorbance. Specifically, the reflectance, transmittance and absorbance of the heater can be adjusted by changing certain design factors, including the grid hole size, the susceptor impedance, the grid geometry, the spacing between the grid and the susceptor and the spacing between adjacent holes. The food items contemplated for cooking in such a package is similar to those noted above, particularly food items which require some amount of surface browning or crisping, such as pizza, fish sticks or french fries. Moreover, the problem of adequately heating the center of these types of foods is not required by this device, due to their relatively thin overall nature. Containers have been also developed which include specially designed covers or lids which are capable of modifying microwave field patterns and which may undergo a change in dielectric constant during microwave heating thereof to alter the heating distribution within the container as heating proceeds. US - A - 4,888,459 (EP - A - 0 271 981) discloses a microwave container which includes a dielectric structure to provide these properties. Specifically, it discloses a container which may include a lid having a single or a plurality of metal plates or sheets located thereon. A region of higher electrical thickness is formed from a dispersion of metal particles in a matrix wherein the dielectric constant of the higher electrical portion is disclosed to be in the range of 25 to 30 for a nonlimiting region. Further, the region may be lossy in character which allows the region, at least initially, to be microwave absorptive, and thus, heat up when exposed to microwave energy. In addition, the region of greater electrical thickness may actually undergo a decrease in dielectric constant during the course of microwave heating. Unfortunately, the region or regions of greater electric thickness disclosed in US - A - 4,888,459 and US - A - 4,866,234 are at least partially interactive with microwave energy. As a result, the region will produce heat during microwave cooking which may not be desired for certain food items, such as pot pies or fruit pies. Furthermore, without the "shut-off" feature, the production of heat may also create a scorching or fire hazard for food items which require an extended cooking time. US - A - 4,972,058 discloses a composite material for generation of heat by absorption of microwave energy. EP - A - 0 382 399 discloses a microwave heating package with a means for modifying microwave energy fields so that the dielectric heating effect within the surface layer of food contained in the package is enhanced relative to the dielectric heating effect in the main portion of the food. So, the surface layer reaches a higher temperature. This prior art deals with the arrangement of apertures to achieve this modifying effect by filtering the microwave energy in order to receive the form of a cut-off propagation. EP - A - 0 291 309 describes a container for holding a body of material to be heated in a microwave oven. The container comprises at least one surface provided with a structure for generating within the container a microwave energy mode of a higher order than that of the container fundamental modes. The structure is formed by an electrically conductive aluminum foil plate positioned on a lid transparent for microwaves. EP - A - 0 242 952 relates to a composite material useful for controlled generation of heat by absorption of microwave energy. This material comprises a dielectric substrate coated with a mixture of an electrically conductive metal or metal alloy in flake form in a thermoplastic dielectric matrix. EP - A - 0 161 739, which corresponds to US - A - 4,656,325 and forms the starting point of the present invention, discloses a microwave heating package with a non-reflecting energy cover that may comprise aluminum flakes in a dielectric substrate. This cover forms metallic islands so that ohmic heating can be obtained by circulating currents. This results in a browning or crispening of the adjacent surface of a food item. Further, the cover acts in a manner analogous with non-reflecting coatings in optics and permits passage of the microwave radiation into the container holding the food item, while substantially preventing escape of microwave radiation reflected from the food item or container bottom. This effect is based on interference of microwaves. The absorbing effect of the cover results in the draw back, that a part of the incident microwave energy is absorbed by the cover so that the total amount of microwave energy entering the cavity formed by the package is reduced. Primary object of the present invention is to modify a package with the above-mentioned features so that either very effective heating of food by means of microwaves can be obtained or a shielding can be formed, wherein the shielding effect can easily be controlled. The above object is achieved by a package with the features of claim 1 and a package produced according to claim 14, respectively. Preferred embodiments are described in the subclaims. Especially, the package body includes a bottom panel and a top panel with side panels joining the bottom and top panel. An impedance matching element is provided on at least one of the panels for impedance matching microwave energy entering the package. The impedance matching element is a contiguous film of thinly flaked material embedded in a dielectric binder which is sized and shaped with respect to the food to cause impedance matching to elevate the temperature of the food in predetermined areas dependent upon the size and spacing of the film without interacting with the microwave energy to produce heat. As a result, the center of a thick food item, such as a pot pie, may be thoroughly heated without scorching or overheating the exterior portions thereof. In the drawings: Figure 1 is a food package including a microwave impedance matching element of the present invention. Figure 2A is an exploded cross-sectional view of the package of Figure 1 taken along lines 2-2. Figure 2B is an exploded cross-sectional view of a second embodiment of the package of Figure 1. Figure 2C is an exploded cross-sectional view of a third embodiment of the package of Figure 1. Figure 2D is an exploded cross-sectional view of a fourth embodiment of the package of Figure 1. Figure 2E is an exploded cross-sectional view of a fifth embodiment of the package of Figure 1. Figure 2F is an exploded cross-sectional view of a sixth embodiment of the package of Figure 1. Figure 2G is an exploded cross-sectional view of a seventh embodiment of the package of Figure 1. Figure 2H is an exploded cross-sectional view of a eighth embodiment of the package of Figure 1. Figure 3 is a cross-sectional view of another embodiment of a food package including a microwave impedance matching element of the present invention. Figure 4A-4B are enhanced microscopic views of the aluminum flake of the present invention. Figures 5A-5C and 6A-6C are enhanced microscopic views of prior art aluminum flakes. Figures 7 and 8 are graphical comparisons of capacitive films including an aluminum flake of the present invention with films including other less effective aluminum flakes. Figure 9 is a graphical comparison of capacitive film including an aluminum flake of the present invention at different binder to flake ratios. Figure 10 illustrates the temperature probe positions within a sample food item used in the examples provided below. Figure 11 is an exploded cross-sectional side view of a second embodiment of the microwave impedance matching element of the present invention. DETAILED DESCRIPTION OF THE INVENTION Microwave cooking of some foods has not been commercially acceptable by consumers for all cooking needs because many thick foods, such as large pot pies or fruit pies, cook faster on the edges than in the middle. The present invention provides a cooking means and food package including the same which impedance matches microwave energy to effectively couple the microwave energy into specific areas of a food item and, thereby, increase the temperature of these areas that normally heat up slowly. Through mathematical analysis, it was determined that the impedance matching means of the present invention is more pronounced on loads with higher dielectric constants and the optimum separation for impedance matching decreases with dielectric constant, but only very little. Impedance matching is accomplished by utilizing a film spaced between a food item and incoming microwave radiation. The presence of the impedance matching film increases the amount of microwave energy directly transferred to the food. For a clearer understanding of the present invention, attention is initially directed to Figure 1. Specifically, Figure 1 illustrates a food package 10. Food package 10 contains a food item 12, shown as a pot pie, within food receiving space 14. A number of additional food items such as fruit pies and stews could also be effectively heated by a package made in accordance with the present invention. Food package 10 includes a top panel 16, side panels 18 and bottom panel 20 which form food receiving space 14 which is substantially transparent to microwave energy and may be constructed from a variety of microwave transparent materials. Preferably, the food package is made from paper or paperboard, but may also be fabricated from a microwave compatible plastic material. Impedance matching member 22 is preferably positioned on top panel 16 over food item 12. By positioning impedance matching member 22 over food item 12, as shown in Figure 1, the microwave energy entering package 10 is impedance matched by member 22 to effectively distribute microwave energy into the center of food item 12 wherein member 22 does not interact with the microwave energy to produce heat. As a result, member 22 is not a heater in the conventional sense, but instead provides a novel means for effectively raising the temperature of the interior of a food item by impedance matching the incident microwave energy acting on the food. Figure 2A clearly shows impedance matching member 22 positioned on the interior surface of top panel 16 over food item 12. Preferably, impedance matching member 22 is positioned from 1/8" to 5/8" above the surface of food item 12. Impedance matching member 22 may be printed or coated directly onto container 10 or it may be previously applied to a separate substrate. The substrate may be paperboard, paper, polyester film or any other microwave transparent material capable of carrying impedance matching member 22. Food package 10 may also be designed in a number of additional configurations, some of which are illustrated in Figures 2B-2H. Specifically, Figure 2B shows package 10 having impedance matching member located on the outside of the package on top panel 16. In addition, impedance matching member 22 may also be placed between different materials. For instance, Figures 2C and 2D illustrate impedance matching member 22 positioned between a substrate 24 and an adhesive layer 26 used to laminate the impedance matching member to the top panel 16 of food package 10. Substrate 24 may be paper, paperboard, or film upon which impedance matching member 22 may be printed or coated. Figures 2E and 2F illustrate additional embodiments in which impedance matching member 22 is embedded or surrounded by a film 28 of resin or ink applied to the surface by a conventional printing process, for example. Further, impedance matching member 22 can be sandwiched by a material 30, such as paper, paperboard, or plastic, which is adhered to a surface by an adhesive layer 26, as illustrated in Figures 2G and 2H. These embodiments are but a few of the many package configurations possible which utilize impedance matching member 22. Figure 3 illustrates yet another possible package configuration 10 wherein impedance matching member 22 is located on a lid of a food tray, rather than on a separate carton, as shown in Figures 1 and 2A-2H. Impedance matching member 22 comprises a film of thinly flaked material embedded or held within a dielectric binder material. Preferably, impedance matching member 22 is shaped to be diametrically smaller than food item 12. The dielectric binder may be chosen from a variety of commercially available binder materials, for example silicone or acrylic binders. Specifically, the preferred dielectric binder is a low loss tangent, high dielectric constant, and high dielectric strength material (all measured at 2.45 GHz). Low loss silicone binders, such as Dow Corning™ 1-2577, and some acrylics, such as the styrene/acrylic Joncryl 611 from Johnson Wax™, may be utilized to provide coatings with the desired impedance matching response without producing detrimental heat in the presence of microwave energy. On the other hand, if a resin with a high loss tangent, such a nitrocellulose, is utilized as the binder material, the resultant impedance matching coating will undergo excessive heating when exposed to microwave energy resulting in a variety of undesirable side effects, such as scorching or melting of the coating substrate. The thinly flaked material of the present invention is essential to achieving advantageous results. The flakes are generally flat and planar and made from a metallic material. It is important that the flake have a length which allows it to lay substantially flat in the binder material. At the same time, the flake should be at a length which allows it to be printed onto a substrate by a conventional printing process, such as gravure printing. Generally, the desired flakes are aluminum metal having an average longest dimension within the range of approximately 8-75 micrometers (µm) and a smaller dimension or width in the range of 5-35 µm. Preferably, the longest dimension is within the range of 10-30 µm. Although aluminum metal is preferred, other metal materials may be equally applicable to the present invention. Referring to Figures 4A and 4B, the preferred flakes of the present invention are shown under magnification. As can be seen, the flakes themselves appear to have a substantially smooth perimeter with a limited number of fragmented flakes present in the binder. The apparent smoothness of a flake may depend upon the degree of magnification. However, describing the flake perimeter as smooth can be defined by comparing it to a flake having a jagged perimeter. Specifically, the smoothness of the perimeter of the flake can be contrasted with a flake which is jagged to the extent that a jagged flake includes a multiplicity of intersecting straight lines to form angles less than 180°. The smooth perimeter of the flake provides a lesser total parametric length than a jagged perimeter. Figures 5A-5C and 6A-6C illustrate prior art metal flakes. It is clear by comparing the flakes shown in Figures 5A-5C and 6A-6C with those shown in Figures 4A and 4B that the flakes shown in Figures 4A and 4B have a smaller parametric length. In addition to length, the thickness of the flake material is also important in obtaining the advantageous features of the present invention. The flake should have a sufficient thickness to maintain flake dimensional integrity and sufficient mechanical strength to endure dispersion in the binder material. On the other hand, the flake material should not be so thick that it no longer is capable of providing close packing between adjacent flakes. Preferably, the flakes have a thickness within the range of 100-500Å. More preferably, the flake has a thickness within the range of about 100-200Å. If the flake material is made of aluminum metal, the preferred aluminum flake is made from aluminum metal by vapor deposition and the thickness should provide an optical density within the range of 1-4. The flake material, also, preferably has an aspect ratio of at least 1000. Such an aspect ratio provides an impedance matching member 22 having an effective dielectric constant of at least 4,000. At such a high dielectric constant, a thin impedance matching member 22 is capable of matching the impedance of the microwave energy present in a microwave oven and in so doing direct the microwave energy more effectively into the interior of the food item held within the package below the impedance matching member 22. When these flakes are slurried in a dielectric binder and printed, the flakes form an archipelago of flat conductive islands that are almost in contact at many locations to form impedance matching member 22. This concentrates the electric fields in the regions between the flakes and greatly increases the amount of electrical energy that is stored. Impedance matching member 22 formed in this manner is for all intents and purposes a non-conductive film with a very high dielectric constant. A quantitative representation of the films potency for impedance matching is expressed in terms of a single dimensionless film parameter, x. Such a representation may be helpful in understanding the advantageous results substantiated below. Specifically, for resistive and capacitive films, the x's are defined as follows: x = σdZ o /2 (resistive film) x = πifε r ε o Z o d (capacitive film) In these equations, Z o is the free-space impedance of the radiation as projected to the plane of the turn, σ is the bulk conductivity of the resistive film, d is the film thickness, i is the square root of negative one (imaginary), f is the frequency, ε o is the permittivity of free space (generally, equal to 8.85x10 -12 Farads/meter), and ε r is the complex, relative dielectric constant of the capacitive film. Again returning to a mathematical representation of the impedance matching member of the present invention, when a film of infinite extent is immersed in free space, the reflection coefficient, R, and transmission coefficient, T, for resistive and capacitive films are: R = -x/(1+x) T = 1/(1+x) For a resistive film, x is real, T is in phase with the incoming radiation, R is 180° out of phase, and the absolute values of R and T sum to one. Since x is a complex number for the capacitive film, the phase of R and T depends on the magnitude of x and the phase of ε r . When summed as complex numbers, T still equals 1 + R, but the sum of the absolute values of T and R becomes greater than one. Since no energy is dissipated in a perfect dielectric, a capacitive film with the same reflection amplitude as a resistive film transmits more radiation. It should be understood that, in the discussion below, the x-value for capacitive films are complex. The portion of incident power dissipated in a resistive film is: A r = 2x/(1+x) 2 while in the capacitive film, the power dissipated is: A c = 2|x|sinδ/(1+|x| 2 + 2|x|sinδ) where δ is the loss angle of the dielectric. It should be noted that a resistive film has a peak absorption of 0.5 at x = 1, and a capacitive film has a peak absorption of sinδ/(1+sinδ) at |x| = 1 . A perfect dielectric (sinδ = 0) has no absorption for any magnitude of x. It should also be noted that these equations are only applicable to thin films, meaning the thickness of the film should be much less than the wavelength of radiation in the film. Power distribution in thin film radiation may be calculated with simple electrical networks. The incoming radiation is represented as source with an output impedance of free space (Z o ), the film is a resistor or capacitor to ground having a value of Z o /2x and the space behind the film is another Z o resistor to ground. When the free space backing is replaced with a dielectric, such as food stuff, the second Z o must be replaced with the impedance of the dielectric (Z d ). Since the ratio of Z d to Z o is 1/ε r ½ for normally incident radiation, a simple circuit representation will yield a transmission coefficient into a dielectric with a capacitive film coating to be: T = 2/(1+2x+ε r ½ ) For a resistive film, x is real so T decrease monotonically with x. If the dielectric is lossy, ε r has a negative imaginary component. Therefore, as ¦x¦ initially increases for capacitive films (x imaginary), the x term starts to cancel the imaginary part of ε r , and T actually increases. Eventually, x will dominate ε r and T will drop, but for a while, the capacitive film improves the impedance match of lossy foods and, as a result, increases the energy input thereto. Once T is known, the portion of the energy transmitted into a dielectric food load can be calculated as the real part of ε r ½ TT*, where T* is the complex conjugant of T. If the impedance matching film of the present invention is separated by a distance L, the absorption of microwave energy by the food item can be greatly increased. Using the transmission line impedance equation to transfer the impedance of the dielectric a distance L through free space to the film, Z d can be replaced by Z d , as a function of L, to give: Z d (L) Z o = [1+ε r ½ itan(k o L)] [ε r ½ +itan(k o L)] where k o is the wave number in free space which equals 2πf(ε o µ o ) ½ and µ o is equal to 4π x 10 -7 henry/meter. By replacing Z d /Z o from Equation (8) in Equation (7) for 1/ε ½ , it has been found that at film-dielectric separations of integer half wavelengths, the capacitive films can shield quite well. With separations of about 1 cm (plus integer half wavelengths) and x's of about 1.0i (or a dielectric constant times thickness for normal radiation at 2.45 GHz of about 0.04 meters), near total absorption may be realized in an infinite load. Using the circuit model explained above, the effective load of the film and a load, for example water, is the parallel combination of the film and the load transferred to the film. Therefore, the inverse of the effective load is the sum of the inverses of the film impedance and the transferred impedance of the load. When eqn. (8) is used to transfer an impedance (Z) as a function of L, the impedance normalized to Z o (and its inverse) trace out a circle in the complex impedance plane that cuts the real axis at |Z|/Z o and Z o /|Z|. At some place along the curve, i.e. at some separation, L, the inverse of the normalized impedance will be 1.0 plus some positive imaginary number, Ni. If a film is chosen where x equals i/N, then the inverse of x is -Ni and the total impedance is Z o which would be a perfect impedance match with no energy reflected. Since the capacitive film of the present invention does not absorb, all the energy ends up as heat in the load. For this reason, it is very effective for heating the interior portions of a high dielectric food item, such as a pot pie or fruit pie. The value of x for total absorption at the proper separation can be represented as the following function of the dielectric constant of the food stuff: x opt = i[|ε r | ½ + |ε r | -½ -2] ½ 2 As a result, for food having high dielectric constants, the best film capacitance for impedance matching depends more or less on the fourth root of |ε r |-1. Therefore, the capacitance is not extremely sensitive to ε r and a single film can work effectively on a large range of food loads. Example 1 The above-note models were experimentally tested in a microwave oven using a ground terminated, circular waveguide as a receptacle for a water load. The wave guide had a diameter of 8.5 cm and a water level of 3.5 cm. Capacitive films made in accordance with the present invention (x = 1.4i and x = 0.8i) were laminated to paperboard and cut in circles with a diameter of just less than 8.5 cm. The circular capacitive films were placed in the waveguide at various levels above the water, and the temperature rise after 2 minutes in a 650 watt microwave oven was noted. This temperature rise was compared to the temperature rise with a bare board at the same location. The results are set forth below in Tables 1 and 2. 1.4i Capacitive Film Separation (cm) Temperature Rise Bare Board (F°) Temperature Rise Capacitive (F°) 1.2 5.9 13.3 2.2 5.1 3.4 5.0 3.8 4.2 0.8i Capacitive Film Separation (cm) Temperature Rise Bare Board (F°) Temperature Rise Capacitive (F°) 1.5 6.5 14.5 2.8 6.0 7.0 7.5 5.4 4.6 It can be seen that the bare board temperature changes decrease slightly with separation. However, when the capacitive film of the present invention is compared with the bare or naked board, the shorter spacing in each instance increased the heat absorption of the water by better than 2. At the intermediate spacing, as expected, there was no significant effect of the capacitive films. Avery Dennison Corporation produces aluminum flakes having aspect ratios of at least 1000 which provide the x-values required for the present invention in films of practical thickness. Specifically, the preferred aluminum flakes useful for the present invention are produced by the Decorative Films Division of Avery Dennison Corporation and have the product designations of METALURE™ L-57083, L-55350, L-56903, L-57097, L-57103 and L-57102. These particular flakes are produced by vacuum vapor depositing a layer of metal on a thin soluble polymeric coating which has been applied to a smooth carrier. Preferably, a biaxially oriented polyester type film is used as the carrier, such as MYLAR™, a product of Du Pont. The metal layer formed on the carrier is stripped therefrom by dissolving the soluble coating. The preferred vapor deposition thickness for aluminum metal gives an optical density of 1-4 before stripping. This provides a flake having the desired shape and dimensions. If the deposited metal films are too thin, the flakes will not be strong enough to prevent curling upon stripping. On the other hand, if the deposited metal film is too thick, the surface of the film tends to give a rough surface to the flake. Following stripping, the metal layer is then mechanically mixed to provide the desired flake particle size while substantially preventing fragmentation of the flake. The flakes generally have an average major dimension or length of 8-75 µm with very few fine flakes having a major dimension less than 5 µm. Preferably, the width of the flake falls within the range of 5-35 µm. Fines tend to keep the surfaces of the flakes apart. As measured by a Dapple Image Analyzer, the following is the average length and width dimensions of the above-noted flakes: Product Designation Average Length µm Average Width µm L-57083 8.6 5.5 L-55350 11.3 6.6 L-56903 17.2 9.7 L-57097 22.0 10.3 L-57103 25.0 12.0 L-57102 75 34.8 While the L-57103 and L-57102 flakes are microwave responsive, these flakes are difficult to coat and are not, therefore, the most preferred flake materials for impedance matching. However, these flakes are the preferred flake materials for providing microwave shielding discussed in greater detail below. The differences between the preferred Avery type flake material and commercially available flake material becomes readily apparent when microscopically viewed. Other commercially available metal flake materials do not have a sufficient aspect ratio and flatness to provide a dielectric constant that is high enough to adequately impedance match, in a thin film, microwave energy entering a food item to evenly heat the center thereof. In order to show this difference, commercially available flake materials were magnified and visually compared with the preferred Avery type flake material to show the distinct differences therebetween. Figures 5A-5C show a STAPA-C VIII type aluminum flake produced by Obron Corp., and Figures 6A-6C show an ALCAN 5225 type aluminum flake material produced by Alcan. It is clear from these photographs taken at both X3,000 and X8,000 that these materials have less surface area than the Avery type flakes shown in Figures 4A-4B. This results in an aspect ratio of only 75-80 for the ALCAN 5225 flake and approximately 200 for the STAPA-C VIII flake. The Avery type flake has a large surface area while also being very thin to provide the Avery flake with a higher aspect ratio, and ultimately a higher dielectric constant when immersed in a binder than other aluminum flake materials. Moreover, the Avery flake has rounded and smooth parametric edges, rather, than the rough edges shown by the conventional flake materials and includes less flake fragments. The aluminum flake material produced by Avery is important to the operation of the impedance matching film of the present invention primarily because of the extremely high dielectric constant provided by these flakes. A performance comparison of the Avery aluminum flake with aluminum flake material produced by other manufacturers clearly illustrates the significant advantages of the Avery type flake material at the same total mass of aluminum. Tests were conducted to the compare the x-values, mathematically described above, of a number of conventional flake materials with one of the Avery flake samples. Example 2 7.78g of Dow Corning 1-2577 conformal coating (5.6g of silicone resin solids in toluene) was mixed with 30.3g of toluene and 1.4g of Hercules ethylcellulose (T-300 grade which was dissolved in 29.7g of toluene). A mixture of 10.77g of Alcan 5225 (an aluminum flake paste at 65% solids in isopropyl alcohol having a particle size of 12-13 µm) and 60g of ethyl acetate was stirred until a uniform dispersion was obtained and then added to the above binder mixture. The resulting formulation was 10% total solids and had a 50/50 ratio of aluminum flake to binder. Sheets of polyester film (Melinex 813/92 from ICI) were coated with the formulation using a series of Bird film applicators. A similar formulation was made by premixing 11g of STAPA-C VIII (aluminum flake paste at 65% solids in isopropyl alcohol having a particle size of 11 µm) with 12.5g of ethyl acetate until the flake was uniformly dispersed. To this was added 7.8g of Dow Corning 1-2577 conformal coating (5.6g of silicone resin solids in toluene), 30.3g of toluene, and 1.4 g of Hercules ethylcellulose (T-300 grade which was dissolved in 29.7g of toluene). The resulting formulation was 10% solid and had a 50/50 ratio of aluminum flake to total binder. This formulation was also applied to a polyester sheet film as described above. A similar mixture was formed using the preferred Avery flake material, L-56903. A 50/50 ratio of aluminum flake to total binder was formed, as described in greater detail below in Example 7. The 2.45 GHz x-values for normally incident radiation (Z o = 377 Ohms) were calculated using, for example, Equations (3) and (4), and network analyzer transmission and reflection measurements on samples mounted crosswise in an S-band waveguide. The results of these three sheet materials are shown in Figure 7 as a function of aluminum coat weight. Figure 7 clearly shows that the use of these conventional aluminum flake materials, rather than a flake material having the characteristics of the Avery flake, is impractical to achieve the impedance matching ability of the present thin film. Specifically, to reach a desired x-value of 0.7i-2.0i, or more preferably, 1.0i-1.8i, 20-40 lbs./3000 sq.ft. of conventional flake would be required. Such an extreme amount of flake material would not easily form a thin film. Further, even at this extremely high level, there is no indication that such a large amount of flake material would actually perform the impedance matching function of the present invention. Additional tests were also conducted to compare the gravure printability of the preferred flake material in both a silicone binder and an acrylic binder with that of a conventional flake material in a silicone binder. Example 3 A coating was made by mixing 5,000g of toluene with 4,000g of aluminum flake (Metalure L-56903 - 10% solids in ethyl acetate). To this was added a mixture of 556g of Dow Corning 1-2577, which is silicone resin (73 % solids in toluene) and 444g of toluene. The resulting formulation was 8 % solids with a 1:1 ratio of aluminum flake and binder solids. The viscosity of the formulation was 22 sec. with a #2 Zahn cup. This formulation was applied to a PET film (grade 813/92 from ICI) on a web fed gravure press at 113 ft./min. using a 100 line cylinder with etched quadrangular cells. Example 4 A coating was made by mixing 3360g of aluminum flake (Metalure L-56903; 10% solids in ethyl acetate) with 1920g of n-propyl acetate. To this mixture was added 108g of Joncryl SCX-611 (an acrylic resin from S.C. Johnson & Sons, Inc.) in 252g of n-propyl acetate and 36g of ethylcellulose (grade N-300 from Hercules Inc.) in 324g of n-propyl acetate. This mixture was diluted to 6% total solids by adding an additional 2,000g of n-propyl acetate. The viscosity of the resulting mixture was 24 sec. with a #2 Zahn cup. The resulting mixture was applied to a PET film using a gravure press, as described above in Example 3, at 125 ft./min. line speed. Example 5 A coating using conventional aluminum flake material was also made by first mixing 3,200g of STAPA-C VIII (a 65% solids paste in isopropyl alcohol) with 2,300g of ethyl acetate and 1,000g of isopropyl acetate until a uniform dispersion was obtained. To this dispersion was added a mixture of 1,250g of Dow Corning 1-2577 (72% solids in toluene) and 2,250g of toluene. The combined formulation was 30% solids and had a viscosity of 17 sec. with a #2 Zahn cup. The resulting mixture was applied to a PET film using a gravure press, as described above in Example 3, at 75-85 ft./min. line speed. The resulting coat weights and x-values at normal radiation at 2.45 GHz for the formulations of Examples 3-5 are provided below in Table 4. Aluminum Flake To Binder Ratio Number of Passes On Press Aluminum Coat Wt. Lb./3,000 Sq. Ft. Capacitive x-Value Effective Dielectric Constant Avery Al flake (Ex. 3) 50/50 1 0.3 0.34i 20,000 2 0.6 1.1i 32,000 3 0.9 1.4i 27,000 Avery Al flake (Ex. 4) 70/30 1 0.3 1.2i 130,000 2 0.6 2.2i 120,000 3 1.0 3.4i 100,000 Obron Al flake (Ex. 5) 70/30 1 1.3 0.09i 2,000 2 3.0 0.20i 2,000 3 4.8 0.31i 1,900 4 6.4 0.41i 1,700 5 8.3 0.53i 1,900 6 10.1 0.63i 1,700 The effect of flake size of the preferred aluminum flake material having the characteristics of the flakes produced by Avery on the x-value is also important in achieving the desired impedance matching characteristics. A number of coating formulations were made using each of the flakes noted above from Avery, Inc., as well as a formulation using the STAPA-C VIII flake from Obron Corp. Example 6 The coating formulation was made by mixing 56g of aluminum flake slurry (Metalure L-55350), which is 10% solids in ethyl acetate, with 32g of n-propyl acetate. To this was added 1.8g of Joncryl SCX-611 (an acrylic resin from S.C. Johnson & Sons, Inc.) in 4.2g of n-propyl acetate and 0.6g of ethylcellulose (grade N-300 from Hercules, Inc.) in 5.4g of n-propyl acetate. This 8% solids formulation, having a 70/30 aluminum flake to binder ratio, was applied to PET film with a Bird bar applicator to obtain the coat weights shown below in Table 5. The general procedure was repeated with the following flake materials: L-57083; L-56903; L-57103; L-57102; and STAPA-C VIII. The results of this comparison are provided below in Table 5 and shown graphically in Figure 8. The results of this comparison show that within the range of flake sizes of the preferred Avery flake, all of which being better than the conventional flake, a flake size of 17 µm provides the consistently best capacitive x-value for impedance matching. The results of Table 5 also illustrate the extreme effective dielectric constant achievable with the present invention, over 18,000, compared to prior materials, only 1,000. Particle Size Aluminum Flake Avg. Length Avg. Width Aluminum Coat Wt. Lbs/3000 sq. ft. Capa. x-value Effective Dielectric Constant L-57083 8.6 5.5 0.7 0.43i 18,000 1.0 0.63i 19,000 1.8 1.07i 18,000 L-55350 11.3 6.6 0.7 0.81i 34,000 1.1 1.25i 34,000 1.8 1.99i 33,000 L-56903 17.2 9.7 0.6 1.41i 70,000 0.8 2.10i 78,000 1.6 4.77i 89,000 2.6 7.56i 87,000 L-57103 25 12 0.4 4.32i 320,000 0.5 4.94i 294,000 1.0 35.05i 1,040,000 1.7 57.67i 1,010,000 L-57102 75 34.8 0.6 0.13i 6,000 0.8 0.46i 17,000 1.6 3.30i 61,000 2.6 10.4i 119,000 STAPA CVIII 15 0.9 0.03i 1,000 1.5 0.05i 1,000 1.9 0.07i 1,100 3.3 0.11i 1,000 Using the preferred flakes, it is also important to utilize the proper flake to binder ratio to achieve the desired x-value. The following tests were conducted to show the effect of the ratio of aluminum flake material in the binder on the x-value. It is assumed that as the amount of binder in the capacitive film is increased the spacing between the flakes will likewise be increased. Generally, the flakes may comprise about 30-80 percent by weight of the film in order to achieve the advantageous effects of the present invention. Preferably, the flakes are present from about 30-70 percent by weight. Example 7 A master batch of aluminum flake coating utilizing a silicone resin as the primary binder and an ethylcellulose as a thickener and secondary binder was prepared. The master batch contained 4.44g of Dow Corning 1-2577 conformal coating (3.2g of silicone resin solids in toluene) and 2.8g of Hercules ethylcellulose (T-300 grade which was previously dissolved in 59.2 g of toluene). To this mixture, 14g of aluminum flake solids (L-56903 in ethyl acetate at 10% solids) was added. Thus, the ratio of aluminum flake to binder was 70/30. (1) 70/30 aluminum flake to binder coatings : 51.5g of the above master batch, which contains 5g of combined solids, was diluted to 100g with toluene. Wet films of this 5% solids formulation were applied to sheets of polyester film (MELINEX 813/92) with Bird film applicators. By using applicators designed to apply 0.0005, 0.001 and 0.002 in. of wet film, it was possible to obtain dried coatings containing 0.4, 0.8 and 1.5 lb/3000 sq. ft., respectively, of aluminum flake solids. (2) 50/50 aluminum flake to binder coatings : To 36.8g of the above master batch (containing 2.5g of aluminum flake, 0.57g of silicone resin and 0.50g of ethylcellulose solids) was added 1.7g of Dow Corning 1-2577 silicone resin solution (1.23g solids) and 0.2g of Hercules ethylcellulose (T-300 grade dissolved in 4.3g of toluene) and 52g of toluene to provide a 5% total solids formulation containing 50% aluminum flake and 50% total binder. This formulation was applied to film using the technique described above to obtain dry coating containing 0.7, 1.2 and 2.0 lb./3000sq.ft. of aluminum flake solids. (3) 30/70 aluminum flake to binder coating : To 22.1g of the above master batch (containing 1.5g of aluminum flake, 0.34g of silicone resin and 0.30g of ethylcellulose solids) was added 3.4g of Dow Corning 1-2577 silicone resin solution (2.46g solids) and 0.4g of Hercules ethylcellulose (T-300 grade dissolved in 8.5g of toluene) and 65.6g of toluene making a 5% total solids formulation containing 30% aluminum flake and 70% total binder. This formulation was applied to film using the above noted technique to obtain dry coatings containing 0.6, 1.0 and 1.3 lb./3000 sq.ft. of aluminum flake solids. The x-values for each of the coatings were calculated from measurements made with an S-band waveguide, as discussed above, and a Hewlett Packard network analyzer (Model 8753A). The results are shown in Table 6 below and graphically in Figure 9. It is readily apparent from these results that as the flake ratio is increased, the x-value per pound of aluminum improves. Aluminum Flake To Binder Ratio Aluminum Coat Wt. Lbs./3000 Sq. Ft. Capacitive x-Value Effective Dielectric Constant 70/30 0.4 0.71i 53,000 0.8 1.58i 59,000 1.5 3.08i 61,000 50/50 0.7 0.61i 18,000 1.2 1.24i 18,000 2.0 2.24i 16,000 30/70 0.6 0.37i 5,000 1.0 0.65i 6,000 1.3 0.91i 6,000 A number of additional tests were conducted using actual food samples to demonstrate the enhanced heating provided by the impedance matching member 22 of the present invention. A food carton similar to carton 10 of Figure 1 was utilized in the following examples. Example 8 An oval shaped impedance matching member 22 was placed 5/8" above a Tyson 18oz Chicken Pot Pie. A control carton was used which was 8 7/8" wide, 6 1/8" deep and 1 1/2" high. The control carton did not include the impedance matching member. A modified carton 10, similar to the carton illustrated in Figure 1, was 1 7/8" high. The oval impedance matching member 22 was 3 1/2" by 2 7/8" wherein x = 1.01i. Each of the runs involved heating the pot pie for 5 minutes, rotating the pot pie 90° and then heating the pot pie for another 5 minutes. Four cooking runs were performed wherein the pot pie was cooked without a box (#1), in the control box (#2), in a box having the whole inside surface covered with impedance matching member 22 (#3), and in a box including the oval shaped member 22 placed on the top panel as shown in Figure 1 (#4). Temperature probes were placed in the pot pie in the positions shown in Figure 10. The results of these runs are shown below in Table 7. Temperature (°F) Position #1 #2 #3 #4 C 91 95 70 153 LI 194 200 192 195 IC 190 192 180 186 RI 197 198 193 182 LC 200 200 195 199 RC 193 187 185 188 LO 192 193 192 193 OC 185 184 192 183 RO 186 188 179 190 Example 9 Another series of tests were run to compare a control carton having no impedance matching member (#5), a rectangular shaped (#6) impedance matching member 3 1/2" x 3" and the oval shaped (#7) impedance matching member 22 from above wherein x = 0.8i. A pot pie was cooked as noted above in Example 8 in each of the cartons, and the results of these runs are shown below in Table 8. Temperature (°F) Position #5 #6 #7 C 94 117 155 LI 195 198 190 IC 192 192 197 RI 186 190 198 LC 199 193 192 RC 182 183 186 LO 186 185 186 OC 188 189 188 RO 180 187 190 Example 10 A test (#8) was also run using a conventional piece of aluminum foil in the same oval configuration provided above with respect to impedance matching member 22 used above in Examples 8 and 9. The aluminum foil oval was elevated 3/8" above a Tyson 18oz Pot Pie. Example 11 A test (#9) was conducted using an impedance matching member 22 with a thickness twice that of the impedance matching members noted above (x = 1.3i + 0.8i) and the same oval configuration provided above. Example 12 A test (#10) was conducted using an enlarged oval impedance matching member 22 having the dimensions of 4" x 4 1/2" wherein x = 1.3. Other conditions were the same as above. Example 13 The distance the impedance matching member 22 having the 3" x 3 1/2" oval dimensions was also adjusted to determine center pie heating (#11). Particularly, the member was placed on the inside top surface of the carton 1/2" over the surface of the pie. The results of Examples 10-13 are provided below in Table 9. Temperature (°F) Position #8 #9 #10 #11 C 64 123 120 155 LI 190 195 198 192 IC 192 185 197 188 RI 192 182 192 180 LC 193 197 198 180 RC 184 182 191 180 LO 187 186 193 187 OC 188 194 195 185 RO 182 184 192 185 Example 14 The dimensions of carton 10 and member 22 were also adjusted to optimize the degree of heating in the center of the pot pie (#12). For example, an open ended carton or sleeve having a length of 9", a width of 6" and a height of 2 1/4" was used to heat a Tyson 18 oz Chicken Pot Pie. The pot pie was resting on three layers of corrugated paper, and the distance between the pie and the impedance matching member was 5/8". The larger oval impedance matching member was used which was 4 1/2" x 4" with x = 1.1i. Example 15 A test (#13) similar to Example 8 was conducted utilizing the same cooking sleeve. However, the oval impedance matching member dimensions were reduced to 2" x 1 3/4" with x = 1.1i. Example 16 Two additional tests (#14 and #15) similar to Examples 8 and 9 were conducted utilizing the same cooking sleeve. However, the oval impedance matching member dimensions were 2 1/2" x 2" with x = 1.1i. Example 17 Finally, a control test (#16) was run with a pot pie similar to that used in Examples 14-16. However, the pot pie was cooked without a carton. The results of Examples 14-17 are provided in Table 10 below. Temperature (°F) Position #12 #13 #14 #15 #16 C 185 147 155 182 79 LI 175 190 190 190 193 IC 170 188 181 192 179 RI 187 183 183 189 182 LC 176 196 196 197 192 RC 176 175 173 184 176 LO 171 187 186 188 186 OC 185 191 180 189 166 RO - 193 184 192 181 Cartons were also tested to determine an optimum size for a rectangular or square impedance matching member which elevates the temperature of a pot pie similar to the advantageous heating provided by the oval design. A series of tests were run on a Tyson 18oz Chicken Pot Pie using a carton similar to the carton used above in Examples 14-17 having a carton depth of 1 5/8", but replacing the oval impedance matching member with a rectangular member 2 1/2" x 2". Table 11 provides the results of three different tests run with the rectangular member (#17, #18, #19, #20). A control test was also run without a carton (#21). Temperature (°F) Position #17 #18 #19 #20 #21 C 152 162 160 187 127 LI 199 186 187 198 194 IC 185 186 174 191 195 RI 191 191 177 188 190 LC 195 192 183 195 188 RC 178 189 162 188 189 LO 186 185 156 188 187 OC 191 183 178 193 186 RO 189 171 171 195 188 As can be seen in each of the results noted above, substantially increased center temperatures for the pot pie were achieved using the impedance matching member of the present invention. The impedance matching member of the present invention may also be useful for altering the relative cooking rates and temperatures of two different items. Such a result may be very effective in complete microwave dinners that include a variety of different foods, each requiring different heating characteristics. For example, the meat portion of a complete dinner may require higher heating temperatures than the vegetable portion. However, to provide the consumer with added convenience, these items are commonly provided in the same packaging tray. The use of the impedance matching member of the present invention for one portion of the tray and not another can cause dramatic differences in temperature. Example 18 Two beakers of water were placed in a 600 watt microwave oven at the same time, one of the beakers on the left side of the oven and one on the right side. Average power absorption from room temperature to boiling was calculated for each beaker. Data was taken for all possible combinations: no impedance matching; left impedance matched, right unmatched; left unmatched, right impedance matched; and both impedance matched. Experiments were conducted for both 100 mL water loads and 400 mL water loads. The results are set forth in Table 12 below. Average Power Absorption (W) Water load (mL) left naked right naked left match right naked left naked right match left match right match 100 252 257 346 190 190 323 260 257 400 270 285 365 208 218 350 291 279 The impedance matched sections of the oven contents heated faster than unmatched sections. However, impedance matching the total contents did not increase the total oven output. Partial impedance matching generally redistributes the heating in the oven. In addition to uniform impedance matching members used for impedance matching radiation into hard to heat regions of a food item, the impedance matching member of the present invention may also be configured in a nonuniform nature to function in a microwave oven similar to a convex glass lens. Figure 11 illustrates an example of a modified impedance matching member 22' within package 10 which is configured similar to a convex optical lens. Such a configuration is useful to further direct microwave radiation to desired areas of package 10. As noted above, the transmission coefficient, T, is a complex number. Therefore, there will be a phase shift through the film represented as: Φ = -tan -1 x If an impedance matching member of the present invention is printed such that the center is thicker than the edges, a decreasing phase shift would be created approaching the periphery of the member. As a result, radiation in the microwave could be focused similar to light through a convex optical lens. Specifically, as in optical lenses, the focal condition occurs due to the phase shift at the center equalling the extra shift due to the larger path depth at the edge, or: tan -1 x = 2π[(h 2 + L 2 ) ½ -1]/λ where h is half height of the lens, L is the focal length, and λ is the wavelength of the radiation. To realize the best lens shape, the lens x-value as a function of y (the distance from the center of a lens), formed in accordance with the present invention, the following equation applies: x(y) = tan{2π[(h 2 +L 2 ) ½ - 1]/λ} - tan{2π[(y 2 +L 2 ) ½ - 1]/λ} In addition to the above-noted advantages of impedance matching, if the x-values of the films are high enough, the film can also act as a shield. Specifically, if the x-value is higher than 10i, for example, the film may function as a shield to reduce the amount of microwave energy reaching a food item placed below the film. For normally incident radiation, the ratio of the electric field amplitude entering a dielectric food stuff with a capacitive film shield at the surface to the field entering without such a shield can be represented as: 1 + ε ½ 1 + 2x + ε ½ where ε is the effective dielectric constant. As evidenced by this relationship, the level of capacitive film depends on the dielectric constant. For typical food stuff having a dielectric constant of 50, the capacitive x-value should be at least 10i. Table 5 provides an example of a flake material and coat weight capable of providing shielding. Specifically, the L-57103 flake, having an average length of 25 µm and a coat weight of 1.0-1.7 lbs/3000 sq.ft. Example 19 Tests were conducted to demonstrate the usefulness of a high x value capacitive film for shielding foods in a microwave oven. Specifically, two paper cups containing 120g of water were each placed in a 700 watt Litton microwave oven. First, each cup of water having no flaked material introduced in the cup was heated in a 700 watt LITTON™ microwave oven until one reached about 200°F. The temperature in each cup was monitored by two Luxtron probes suspended at fixed, reproducible positions in the water. The average heat dissipation in watts was calculated for each cup of water from the average temperature rise and heating time. Next, aluminum foil patches were glued on the bottom and the sides of one of the cups designated at cup B. Again, the average power dissipation was calculated. This procedure was conducted two more times by replacing the aluminum foil patches with a capacitive film having an x-value of 1.5i and 20i, respectively. The results are set forth in Table 13 below. Cup Test 1 Test 2 (aluminumfoil) Test 3 (x = 1.5i) Test 4 (x = 20i) A 222 W 273 W 220 W 275 W B 246 W 137 W 238 W 169 W As can be seen by these results, the 1.5i film had little influence on the power dissipation when placed at the surface of the container. However, the aluminum foil provides significant shielding illustrated by the reduction of power dissipation in cup B in Test 2. Test 4 illustrates that a 20i film also provides shielding and also demonstrates that, by using capacitive films made in accordance with the present invention, the amount of shielding can be controlled by adjusting the x-value of the film.

Claims: Package (10) for storing and microwave heating food, wherein the package (10) is at least partially substantially transparent to microwave energy and forms a food receiving cavity including a bottom panel (16), a top panel (20), and side panels (18) joining the bottom panel (16) with the top panel (20), wherein the package is at least partially provided with flakes embedded in a dielectric binder, characterized in that an impedance matching means comprising a contiguous capacitive film of the flakes embedded in a dielectric binder is provided on a surface of at least one of the panels (16, 18, 20) for impedance matching microwave energy entering the package (10) without interacting with the microwave energy to produce heat. Package (10) according to claim 1, characterized in that the flakes are generally planar, and that the flakes consist of a metal material, preferably of aluminium. Package (10) according to claim 1 or 2, characterized in that the flakes have a longest average dimension within the range of about 8-75 µm and a thickness within the range of about 1 x 10 -8 to 5 x 10 -8 m, preferably within the range of about 1 x 10 -8 to 2 x 10 -8 m and/or that the flakes have an aspect ratio of at least about 1000. Package (10) according to any one of the preceding claims, characterized in that the flakes are present at a coat weight within the range of about 0,48-4,24 g/m 2 (0,3-2,6 lb./3000 sq. ft.), preferably at a coat height within the range of about 0,48-2,93 g/m 2 (0,3-1,8 lb./3000 sq. ft). Package (10) according to any one of the preceding claims, characterized in that the flakes comprise about 30-70 percent by weight of the film, preferably 70 percent by weight of the film. Package (10) according to any one of the preceding claims, characterized in that the impedance matching means has an effective dielectric constant of at least 4000. Package (10) according to any one of the preceding claims, characterized in that the impedance matching means is positioned on the top panel (20) above the food, preferably about 0,32 cm (1/8 ") to 1,6 cm (5/8 ") above the food. Package (10) according to any one of the preceding claims, characterized in that the impedance matching means is diametrically smaller than the food held within the package (10), and preferably wherein the impedance matching means is oval shaped. Package (10) according to any one of the preceding claims, characterized in that the surface of at least one of the panels (16, 18, 20) comprises paper or paperboard or that the substrate of the film is paper, paperboard or plastic film. Package (10) according to any one of the preceding claims, characterized in that the impedance matching means is sized and spaced with respect to the food to cause impedance matching to elevate the temperature of the food by increasing the amount of microwave energy directed to the food in at least a predetermined area thereof dependent upon the size and spacing of the film without interacting with the microwave energy to produce heat. Package (10) according to any one of the preceding claims, characterized in that the film has a capacitive x-value within the range of about 0,7i - 2,0i. Package (10) according to any one of the preceding claims, characterized in that the impedance matching means is provided on an extended surface of at least one panel (16, 18, 20) for impedance matching microwave energy entering the package (10), wherein the impedance matching means is convex such that a centre thereof has a thickness greater than the thickness at the periphery thereof to focus impedance matched microwave energy toward the food to elevate the temperature of the food by increasing the amount of microwave energy directed to the food in an area corresponding to the size of the impedance matching means and spacing of the impedance matching means from the food without interacting with the microwave energy to produce heat. Package (10) according to any one of claims 1 to 9, characterized in that the impedance matching means are provided for shielding a food item (12) from microwave energy positioned proximate thereto, wherein the capacitive film is a composite material in the form of a contiguous film of generally planar flakes embedded in a dielectric binder in an amount sufficient to reduce microwave energy reaching the food item (12) when said composite material is positioned proximate thereto, wherein preferably a capacitive x-value of the composite material is greater than 10i and/or wherein an effective dielectric constant of the composite material is at least about 100000. The package (10) according to any one of the preceding claims, characterized in that said film of flakes is formed by the steps of: a) vapour depositing a layer of aluminium metal preferably with an optical density within the range of about 1 to 4 on a soluble polymeric coating applied to a carrier; and b) stripping the layer from the carrier.

Inventors: HABEGER CHARLES C JR, JOSEPHY KARL, POLLART KENNETH A, RETTKER JAMES P, THOMAS RICHARD N, HABEGER, CHARLES C., JR., JOSEPHY, KARL, POLLART, KENNETH A., RETTKER, JAMES P., THOMAS, RICHARD N.
Applicants: FORT JAMES OPERATING COMPANY
Application year: 1994
Main classification: B65D81
IPC codes: A23L1, A47J27, B65D81, A23L3, A47J36